The behavior of the probability density \(\rm |\Psi |^{2}\)  (from eq. (REF )) in terms of the volume function \(\rm V\)  and the scalar field \(\rm \phi _{2}\)  is presented in Fig. REF . Also, the evolution of \(\rm |\Psi |^{2}\)  is shown for different values of the factor ordering parameter \(\rm Q\) ; and actually, in all panels the probability density dies away as \(\rm V\)  and \(\rm \phi _{2}\)  evolve. An expected outcome already reported in [1]}, [2]}, [3]}, [4]}, [5]}. Moreover, when \(\rm Q\ll 0\)  then \(\rm |\Psi |^{2}\)  tends to behave similar to the isotropic case [2]}.
